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Measurements of fractionated gaseous mercury concentrations over northwestern and central Europe, 1995-99

Authors:
  • Institute of Geochemistry, Chinese Academy of Sciences, Guiyang 550002

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Although it makes up only a few per cent. of total gaseous mercury (TGM) in the atmosphere, the fraction of oxidised (divalent) mercury plays a major role in the biogeochemical cycle of mercury due to its high affinity for water and surfaces. Quantitative knowledge of this fraction present in mixing ratios in the parts-per-10(15) (ppq) range is currently very scarce. This work is based on approximately 220 data for divalent gaseous mercury (DGM) collected during 1995-99 in ambient air. Over the course of the measurements, the sampling and analytical methods were modified and improved. This is described here in detail and includes transition from wet leaching and reduction procedures to thermo-reductive desorption, the use of annular as well as tubular denuders and adoption of an automated sampling system. The concentration of DGM exhibited a strong seasonal behaviour in contrast to atomic gaseous mercury, with low values in winter and maximum values in summer. The DGM/TGM ratios were frequently found to be below the detection limit (< or = 1%) and in the range 1-5%. A trend of diurnal DGM patterns was observed and implies photolytically induced sources. Scavenging of DGM during rain events was also noticed.
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Measurements of fractionated gaseous mercury concentrations over
northwestern and central Europe, 1995–99†
Jonas Sommar,* Xinbin Feng, Katarina Ga
˚rdfeldt and Oliver Lindqvist
Inorganic Chemistry, Department of Chemistry, Go
¨teborg University, 412 96 Go
¨teborg, Sweden.
E-mail: sommar@inoc.chalmers.se
Received 1st April 1999, Accepted 12th July 1999
Although it makes up only a few per cent. of total gaseous mercury (TGM ) in the atmosphere, the fraction of
oxidised (divalent) mercury plays a major role in the biogeochemical cycle of mercury due to its high anity for
water and surfaces. Quantitative knowledge of this fraction present in mixing ratios in the parts-per-1015 (ppq)
range is currently very scarce. This work is based on #220 data for divalent gaseous mercury ( DGM ) collected
during 1995–99 in ambient air. Over the course of the measurements, the sampling and analytical methods were
modified and improved. This is described here in detail and includes transition from wet leaching and reduction
procedures to thermo-reductive desorption, the use of annular as well as tubular denuders and adoption of an
automated sampling system. The concentration of DGM exhibited a strong seasonal behaviour in contrast to
atomic gaseous mercury, with low values in winter and maximum values in summer. The DGM/TGM ratios were
frequently found to be below the detection limit (1%) and in the range 1–5%. A trend of diurnal DGM patterns
was observed and implies photolytically induced sources. Scavenging of DGM during rain events was also noticed.
Dry adsorption methods to trap oxidised mercury in flue
Aim of investigation
gases rely on the same principle. Oxidised mercury, ‘HgCl2’,
Mercury is the only air pollutant predominantly present in is complexed to [HgCl3]or [ HgCl4]2and retained as the
atomic form (Hg0). Owing to high detection sensitivity, it is complex anion in a KCl matrix. The diusion denuder
possible to monitor roughly background sub-ppt concen- method10 separates gases from particles based on the fact that
trations in the atmosphere with direct absorption methods.1they diuse much faster than particles. For sampling purposes,
For oxidised mercury forms present in the parts-per-1015 (ppq) the gas has to be sucked along a surface that acts as a sink
range in ambient air, accumulative sampling is required. for the specific gas of interest. Numerous coatings can act as
Besides CH3HgX, (CH3)2Hg and Hg0, speciation of gaseous a sink for gaseous divalent mercury compounds but not for
mercury is not obtained, only fractionation. Recently, eorts elemental mercury, such as alkali metal hydroxides, halides
have been made to determine the fraction of oxidised (divalent) and chromates.11 The use of KCl is mainly due to its high
gaseous mercury in the atmosphere.2–5 Normally, this is rep- deliquescence point. The compound traps DGM compounds
resented by reactive gaseous mercury (RGM ). The term is, such as HgCl2and CH3HgCl.2
however, media-dependent and accordingly depends on HgIIaWe have previously published a paper on the applicability
in the aqueous phase, defined by Brosset.6In the following, of KCl denuders to sample and determine RGM in ambient
divalent gaseous mercury ( DGM ) will be used instead and air.2In the present paper, a data set of ambient air RGM,
only when it is appropriate will the term RGM be given. Even DGM and TGM samples from 1995 to date is presented. Over
though DGM makes up only a small portion of the total the course of the measurements, the method was modified and
gaseous mercury ( TGM ) in the atmosphere, it plays an improved in order to make the sampling less strenuous and
important role in the biogeochemical cycle of mercury in the time-consuming and achieve higher time resolution. This
environment due to its high solubility in water and easy includes transition from wet leaching and reduction procedures
deposition back to terrestrial ecosystems by both wet and dry to thermo-reductive desorption,12 the use of annular as well
processes. DGM exhibits dry deposition velocities similar to as tubular denuders and modifications of the technique aimed
those of HNO3
4while the corresponding figure for Hg0is at integration and automation. The dierent techniques are
several orders of magnitude lower. Modelling studies over briefly described and commented upon, being used in overlap
various spatial scales have shown that even trace amounts of during transition periods.
DGM species may control the overall deposition of mercury.7,8
However, further advancement of mercury modelling is limited
by the lack of data on the mercury composition in the
Description of experimental procedures
atmosphere. KCl coated denuders
The earliest evidence for the presence of ppq concentrations
of RGM in ambient air was presented by Brosset.9Using a The denuders were made from quartz or borosilicate glass
high flow refluxing mist chamber, Stratton and Lindberg3,4 tubes. In addition to tubular denuders (Ø#6 mm), annular
were able to obtain diurnal-resolved RGM in ambient air. denuders consisting of two coaxial quartz tubes with #1mm
Representative samples collected corresponded to a detection spacing and with sandblasted annulus walls were also
limit of 1 ppq RGM in ambient air. employed. The cleaning of the tubes and application of a
methanolic KCl solution to the walls were performed as
described previously.2Both ends were cleaned with doubly
†Presented at AIRMON ’99, Geilo, Norway, February 10–14, 1999.
J. Environ. Monit., 1999, 1, 435–439 435
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de-ionised water (Millipore, Milli-Q). The eective KCl coated always present. The generator euent was then diluted to a
suitable concentration by adding carrier gas.length was 50 and 20 cm for tubular and annular denuders,
respectively. The denuders were repeatedly ‘blanked’ by heat-
ing in mercury-free inert gas until low long-term blanks were Sampling set-up
obtained. Denuders that were to be exposed were generally The collection eciency of the divalent species has been shown
‘blanked’ shortly before collection started. to be near-quantitative.2Therefore, most of the DGM and
RGM measurements were performed with single collectors
Determination of mercury only. Usually, about 1–1.5 m3samples were collected in the
Divalent gaseous mercury. Mercury trapped in the denuders KCl denuder. The tubular and annular denuders were main-
was determined either by leaching or thermal desorption. tained at a flow of 0.7–1 and 6 –9 l min1, respectively. The
Borosilicate denuders were only analysed by the former method denuders were mounted vertically with a downturned funnel
whereas denuders made from quartz were subject to testing at the inlet to protect them from precipitation. In about 60%
with both methods. The extraction solution, suprapure grade of the sampling events TGM was co-sampled with DGM.
HCl (Merck), was diluted to 1.0 M with Milli-Q water and
further purified following the procedure previously described2Manual sampling. The assembly for manual sampling of
before being used. Divalent mercury molecules were extracted divalent mercury is given in Fig. 1. Denuders mounted verti-
as their chloro complexes. The leachates were analysed for cally at least 1 m above ground were generally heated at
both RGM and DGM. DGM was obtained after oxidising 40 –50 °C to avoid KCl deliquescencing during sampling. By
the leachate with BrCl followed by reduction with having a negligible pressure drop, the volume exposed to
NH2OH·HCl and eventually with SnCl2and determined by the denuder was obtained by simply using a gas meter
cold vapour atomic fluorescence spectrometry (CVAFS) (Schlumberger) connected downstream.
(Brooks Rand CVAFS-2 Mercury Analyzer or PSA
Millennium Merlin Mercury Analyser). In the former case, a Automated sampling. An automated sampling system for
dual amalgamation step was employed. DGM based on the thermo-reduction desorption principle was
The set-up used to determine mercury by thermal desorption also used. The configuration shown in Fig. 2 is generally
is described below. During analysis or ‘blanking’ of the KCl adopted from the Tekran Model 1130P system (Tekran,
denuder, it was heated externally from a NiCr resistance Toronto, Canada). A heated ( 50 °C) annular denuder with the
ribbon. The temperature (<700 °C) and time were set to the eective KCl coated length enclosed in an oven equipped with
grade of contamination of the denuder. By desorbing at 450 °C, a cooling fan was used to collect DGM. The denuder was
generally >90% of mercury trapped was released in a few connected with short, cleaned Teflon transfer lines to a pump
minutes.12 Samples were generally treated at 450 °C for 10 min. and CVAFS (Tekran 2537A Mercury Vapour Analyzer) unit.
Collectors made of borosilicate were also heated to a few The working principle of the CVAFS system has been described
hundred degrees to attain low blanks. During sample analysis, by Schro
¨der et al.14 The surface temperature of the denuder
mercury species desorbed were pyrolysed before preconcen- was controlled with a set-point controller ( Eurotherm 2416 )
tration on an analytical column with gold-coated quartz beads including time-regulated heating and cooling plug-ins. The
secured with quartz wool plugs. The pyrolyser consisted of flows through the denuder were synchronised with the tempera-
quartz beads in a quartz column maintained at 900 °C. The ture as well as with the CVAFS unit’s sampling cycles using
gold trap was heated in a short pulse to 500 °C and atomic Tekran accessories (1110 Synchronized two port sampling
mercury released was detected by CVAFS (Brooks Rand unit, 1120 Standard Addition Controller). This unit was
CVAFS-2 Mercury Analyzer or Tekran 2537A Mercury continuously sampling ambient air at 1.5 l min1. During
Vapour Analyzer). The output signal from the detector of the preconcentration of DGM, when an additional gas flow of
PSA or Tekran instrument was acquired on a portable #4.5 l min1passes through the denuder, the CVAFS unit
computer. simply detects Hg0. A few cycles before desorption, the inlet
of the denuder was blocked with mercury-scrubbed ambient
Total gaseous mercury. TGM was collected on gold filled air. Hence, the detector only experienced the influence of
quartz tubes (gold traps) either manually or automatically by
a field-portable instrument ( Ekoservis Gardis-1A or Tekran
2537A Mercury Vapour Analyzer). The gold traps were ana-
lysed as described above. Calibration of the instruments was
achieved by injecting certain amounts of elemental mercury
into the analytical system. Mercury was delivered as acidic
aliquots into the PSA instrument and as nitrogen gas saturated
with mercury into the other instruments. The Tekran instru-
ment also exhibits an internal calibration system with a
permeation source.
Laboratory testing of KCl denuders
A detailed description of the HgCl2generation system has
been given previously.2The generation rate is highly dependent
on the temperature and flow of the carrier gas. The parts of
the system upstream of the delivery point have to be completely
heated to a temperature exceeding that of the bath to avoid
condensation. The composition and stability of the source
were tested by connection to an on-line fractionation system
normally used for flue gases.13 The gas stream was pyrolysed
at 600 °C in a quartz cell and detected by Zeeman-eect
electrothermal AAS (Semtech 2000 Mercury Analyzer) at the
Fig. 1 Schematic diagram of set-up for manual sampling with
denuders.
same temperature. A few per cent. of elemental mercury was
436 J. Environ. Monit., 1999, 1, 435–439
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Fig. 2 Schematic diagram of set-up for automated fractionation of
gaseous mercury. The flow indicated by the dark-coloured lines to
the left of the denuder is active during preconcentration while the
flow indicated by the light-coloured lines acts to block the denuder
from ambient air during thermal desorption.
mercury zero air. During desorption, the temperature of the
denuder was ramped to 450 °C and, consequently, DGM
trapped was released, pyrolysed and detected. After the
denuder had been allowed to cool down, preconcentration was
resumed. The internal blank of the denuder was intermittently
checked by passage of mercury zero air during the whole
Fig. 3 Locations of European sampling sites.
sampling period followed by thermal desorption. In the most
recent measurements, deposition of coarse particles on the
denuder was prevented by passing ambient air through a Analytical performance of the methods
cyclone (2.5 mm aerodynamic diameter cut-o).
During 1996, two parallel sampling lines were run with dual
leaching analysis and the variations were in the range up to
Sampling sites 30%. The DGM method blank is generally 15–35 pg and as
Air samples were taken manually from 1995 and automatically low as 10 pg can be obtained for RGM if care is taken to
since 1998. Sampling was performed during two international avoid every possible contamination. Leaching of denuders
intercomparison exercises at Mace Head, County Galway, treated with or without repeated heating after a new coating
Ireland, and at Sasseta, Tuscany, Italy, during September 1995 had been applied showed that heating was necessary to elimin-
and June-July 1998, respectively, involving groups from North ate initial contamination. The use of borosilicate tubes, how-
America and Europe. ever, prevented high temperatures from being used. As it was
The sampling sites in Sweden were located around the city a component of all the solutions used, distillation of the
of Go
¨teborg (58°N12°E) situated on the west coast. About suprapure grade HCl from mercury induced by SnCl2addition
65 samples were exposed at the Brottka
¨rr site 15 km south- was also found to be important.2Contribution from reagents
west during 1995–97. About 25 samples were collected outside gives the DGM method a 5–20 pg higher blank compared
the building of the Department of Chemistry in the urban with that of RGM. The detection limit, based on 3sof the
area of Chalmers. The S:t Jo
¨rgen site is located 15 km north, method blanks, varies between 5 and 15 pg, corresponding to
where a combustion simulator is operated with mercury injec- air concentrations of <2 ppq.
tion for research purposes. Samples were taken outside the The analytical precision of field samples by the thermal
simulator building. Measurements of DGM were also per- method was similar to that described above ( 5–40% variability,
formed within the Mercury Over Europe/Mediterranean triplicate samples, n=7 ). The regenerative use of thermal
Atmospheric Mercury Cycling (MOE/MAMCS) Project. denuders makes the blank smaller and less variable without
MOE/MAMCS is a multi-year project set-up in 1998, which influencing the collection eciency. Typical values of the blank
includes air sampling at ten sites in Western and Southern and detection limit were a few picograms for each based on
Europe. Some results are reported from the Ro
¨rvik site located field blanks. The internal blank of the annular denuder
35 km south-west of Go
¨teborg. was higher, but could be suppressed to 5–10 pg during auto-
The locations of the European sampling sites are shown mated sampling with repeated heating cycles. The detection
in Fig. 3. limit of the thermal methods corresponds typically to DGM
concentrations of <1 ppq.
The sampling data were screened from outliers. Those
Results and discussion
generally encountered resulted from passivation of gold traps
during field measurements and mainly influenced TGM (alsoIn the following, the concentrations given were calculated
based on the molar weight of atomic mercury; hence, the DGM during automated sampling), giving reduced concen-
trations of <100 ppq of the former. About 10% of themixing ratios are slightly overestimated for RGM and DGM.
TGM data presented here were averaged to cover RGM/DGM automated and <2% of the manually collected RGM/DGM
samples were rejected.sampling periods.
J. Environ. Monit., 1999, 1, 435–439 437
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Table 1 Summary of mixing ratios of RGM, DGM and TGM obtained in ambient air at European sites, 1995–1999. The values in italic type
indicate that most of the single samples grouped together were below the detection limit given in Fig. 4
RGM( ppq ) DGM( ppq ) DGMa/TGM (%)
Site Season Method x
:±snx
:±snx
:±sn
Brottka
¨rr All Manual leaching 3.4±2.9 45 4.2±4.0 19 1.7±1.6 32
Summer 4.3±3.1 30 5.0±4.2 15 2.2±1.7 19
Winter 1.5±1.0 15 1.3±0.6 40.8±0.7 13
Ro
¨rvik Winter Manual heating 2.6±2.4 30 1.1±0.9 20
Winter Automated heating 1.0±1.0 34 0.5±0.7 34
Summer Manual heating 3.0±3.1 14 1.7±1.8 13
Summer Automated heating 3.9±2.1 21 2.5±1.3 21
Chalmers Summer Manual leaching 16.0±2.1 3 6.9±2.1 3
Summer Manual heating 5.3±2.5 10
Winter Automated heating 1.0±0.4 13 0.4±0.2 13
S:t Jo
¨rgen Summer Manual leaching 8.7±5.4b20b
Mace Head Summer Manual leaching 9.1±2.9 4 3.0±0.9 4
Sasseta Summer Manual heating 2.1±0.9b14b
aIn Brottka
¨rr data, RGM/TGM is displayed. bIncludes duplicate or triplicate exposed samples.
Intercomparison with other methods to determine oxidised the samples were analysed for both RGM and DGM. The
latter was found to be higher using a one-way analysis ofgaseous mercury
variance test (F=0.46, P<0.06). RGM and DGM were well
The methods currently available to fractionate/speciate correlated with each other (r=0.92, P<0.0001 ) but not with
mercury in ambient airdenuder-based techniques and mist TGM (P=0.21). As shown in Table 1, the dierence was more
chambers—were intercompared during the start-up phase of pronounced during the summer period. The RGM fraction is
the MOE/MAMCS project in Sasseta. Owing to the scarce considered to represent inorganic compounds, since even the
data set, it was dicult to rank the dierent methods. However, most stable inorganic mercury compounds in aqueous solution
it can be concluded that they generally produce relatively have been found to be easily reduced by SnCl2. On the other
similar results with variability up to 30–40%. The complete hand, CH3HgCl(aq) is not reduced by SnCl2and does not
data set including TGM and particulate Hg data will be belong to the RGM fraction.15 This implies the presence of
published elsewhere.15 The results obtained by manual tubular gaseous monomethylated mercury species in ambient air.
and automated annular denuders were intercompared during However, other methods which can exclusively identify such
one campaign at Ro
¨rvik. The data were significantly correlated compounds in air (mist chambers15 and graphitised carbon
(P<0.10, n=9) but diered occasionally in magnitude (within traps16,17 ) have to be used during such speciation.
a factor of 2). The results obtained with annular denuders The concentration of oxidised gaseous mercury exhibited a
were consistently lower. strong seasonal behaviour (P<0.01) with low values in winter
and maximum values in summer. The concentration during
Concentrations of RGM and DGM in air the winter period often dropped below the detection limit (1–2
ppq). This trend has also been observed by Lindberg
In Table 1, the complete set of over 200 data is categorised
and Stratton4and was attributed to seasonal dierences in
into location, season and analytical method. The most extens-
air stagnation and chemical kinetics. Extensive continental
ive data set is from Brottka
¨rr and covers three years, and is
European TGM measurements imply that Hg0is predomi-
displayed in Fig. 4. Exposed denuders were analysed after
nantly sink- rather than source-modulated,6,9,18 –20 which is
manual leaching. RGM was determined throughout the whole
characteristic of atmospheric trace gases removed by oxidation
campaign while DGM was determined occasionally. Samples
processes. Higher oxidant concentrations during summer lead
were usually exposed on a diurnal basis with a flow rate of
to faster oxidation and to a summer minimum of TGM. The
about 700 ml min1. The average level of DGM measured
intensified oxidation process contributes to increased concen-
was 4.2 ppq compared with 3.4 ppq for RGM. Nineteen of
trations of DGM and subsequently enhanced deposition21, 22
of the highly surface-reactive oxidised mercury forms.
However, the role of dierent photolytically induced gas-phase
oxidants has not been shown in any detail.23 In its extreme
manifestation, when high concentrations of oxidants build up
during polar sunrise in the Arctic, fast depletion of elemental
gaseous mercury occurs.24
During winter periods, the frequency of precipitation
increases from 20 to 40% and leads to enhanced scavenging
of oxidised mercury. RGM/DGM was measured during three
rainfall events during summer 1996 and indeed oxidised gase-
ous mercury was found to decrease on average by #60% for
both fractions. TGM showed no consistent variation during
the same period of time. The limited amount of oxidised
mercury collected on the tubular denuders did not allow any
diurnal resolution of the measurements. The introduction of
high-flow annular denuders enabled the same amount to be
collected during a few hours. Fig. 5 shows automated 6 h
measurements of DGM and Hg0at the Chalmers site during
Fig. 4 Time–concentration behaviour of RGM/DGM at Brottka
¨rr
the shift between January and February 1999 (a data series
during 1995–97. The bars given indicate detection limit for each
fraction.
without any significant passivation of gold traps).
438 J. Environ. Monit., 1999, 1, 435–439
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definitely not the case for RGM/DGM. As it is being measured
extensively within the MOE/MAMCS campaign and else-
where, quantitative knowledge of RGM/DGM is, however,
likely to be extended in the near future.
Acknowledgements
This study was initiated by Zifan Xiao, whom we greatly
acknowledge together with Shiqiang Wei. This research was a
contribution to the ‘Mercury species over Europe’ project
being carried out in the specific RTD program sponsored
by the European Community under contract number
ENV4-ET97–0595.
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>3 between extreme figures, were reported in the US data.4
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areas of vegetation significantly by dry deposition. The current
database of TGM is now fairly well established, which is Paper 9/02729G
J. Environ. Monit., 1999, 1, 435–439 439
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... Automatic methods give online data of GEM. Commercially available Tekran gas phase mercury analysers and Gardis analysers are examples of such samplers (Urba et al., 1995;Sommar et al., 1999;Pandey et al., 2011). In the manual gold trap method, GEM is collected on a gold trap which is generally a quartz tube filled with mixture of quartz and small pieces of gold wire at very low flow rate (generally ~0.5 L/min). ...
... This protects contamination of gold cartridges from particulate matter in the stream. GEM so collected is then thermally desorbed and detected in an integrated cold vapor atomic fluorescence spectroscopy (CVAFS) detector (Tekran, 1998;Sommar et al., 1999). For this purpose, the instrument has two parallel gold cartridges which are operated alternatively for sampling and desorption on 10 minute interval at a flow rate of 1.5 L/min. ...
... The collected mercury is detected by SnCl 2 -CVAFS method. In the denuder methods, either tubular (Shiqiang et al., 1997;Sommar et al., 1999;Munthe et al., 2001;Wangberg et al., 2001) or annular denuder (Munthe et al., 1999Lindberg et al., 2002) is used to trap mercury species. Fig. 3 shows a typical annular denuder for automated methods. ...
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Mercury (Hg) is a highly toxic metal, which is known as a global pollutant due to its ability to undergo long-range transport in the atmosphere. Methylated mercury can pose serious adverse effects on human health and environment. Mercury is emitted into the atmosphere by various natural and anthropogenic sources. The largest anthropogenic source of mercury is coal combustion, which contributes ~62% of global emissions. Total global emissions of atmospheric mercury are estimated to be 5600 Mg/year from natural and anthropogenic sources, respectively, contributing around 37% and 63% of total atmospheric mercury. About 40% of global anthropogenic emissions are contributed by East and Southeast Asia with the largest emissions from China (75%) followed by South America and Sub-Saharan Africa. Latter regions are mainly responsible due to increase in artisanal and small scale gold mining. The present estimates of mercury emissions have large uncertainties in global budget, which are mainly due to lack of knowledge of mercury exchange between various components of ecosystem with its speciation in spatial and temporal distribution. Special efforts are needed in the regions of growing economy especially in South Asia where atmospheric mercury is almost unattempted. In order to reduce uncertainties and get more realistic emission figures, there is need to develop an extensive monitoring network to measure various forms of mercury in air, soil and aquatic systems in south Asia. Controlling the emissions of global atmospheric mercury is a big challenge to the scientists and policymakers. Probably, it can be achieved by focusing on implementation of the available technologies and by developing new technologies for mercury removal through developing an extensive partnership between industries and governmental organizations.
... In 2000, Steffen et al. [24] reported on the use of a cold regions pyrolysis unit manufactured by Tekran to allow for measurement of total gaseous mercury, while simultaneously measuring GEM. Their measurements were conducted during a Hg depletion event in the Arctic at Alert, Nunaurt, Canada. ...
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This review focuses on providing the history of measurement efforts to quantify and characterize the compounds of reactive mercury (RM), and the current status of measurement methods and knowledge. RM collectively represents gaseous oxidized mercury (GOM) and that bound to particles. The presence of RM was first recognized through measurement of coal-fired power plant emissions. Once discovered, researchers focused on developing methods for measuring RM in ambient air. First, tubular KCl-coated denuders were used for stack gas measurements, followed by mist chambers and annular denuders for ambient air measurements. For ~15 years, thermal desorption of an annular KCl denuder in the Tekran® speciation system was thought to be the gold standard for ambient GOM measurements. Research over the past ~10 years has shown that the KCl denuder does not collect GOM compounds with equal efficiency, and there are interferences with collection. Using a membrane-based system and an automated system—the Detector for Oxidized mercury System (DOHGS)—concentrations measured with the KCl denuder in the Tekran speciation system underestimate GOM concentrations by 1.3 to 13 times. Using nylon membranes it has been demonstrated that GOM/RM chemistry varies across space and time, and that this depends on the oxidant chemistry of the air. Future work should focus on development of better surfaces for collecting GOM/RM compounds, analytical methods to characterize GOM/RM chemistry, and high-resolution, calibrated measurement systems.
... The chemical speciation of other atmospheric bulk mercury species, besides gaseous Hg 0 , including all oxidized mercury compounds, has been more challenging. GOM is conventionally collected using KCl-coated annular denuders 7 , where oxidized mercury species (such as mercuric chloride [HgCl 2 ]) are complexed as anions ([HgCl 3 ] − and [HgCl 4 ] 2− ) and incorporated within the KCl matrix 8 . ...
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Mercury is an important global toxic contaminant of concern that causes cognitive and neuromuscular damage in humans. It is ubiquitous in the environment and can travel in the air, in water, or adsorb to soils, snow, ice and sediment. Two significant factors that influence the fate of atmospheric mercury, its introduction to aquatic and terrestrial environments, and its bioaccumulation and biomagnification in biotic systems are the chemical species or forms that mercury exists as (elemental, oxidized or organic) and its physical phase (solid, liquid/aqueous, or gaseous). In this work, we show that previously unknown mercury-containing nanoparticles exist in the air using high-resolution scanning transmission electron microscopy imaging (HR-STEM). Deploying an urban-air field campaign near a mercury point source, we provide further evidence for mercury nanoparticles and determine the extent to which these particles contain two long suspected forms of oxidized mercury (mercuric bromide and mercuric chloride) using mercury mass spectrometry (Hg-MS). Using optical particle sizers, we also conclude that the conventional method of measuring gaseous oxidized mercury worldwide can trap up to 95% of nanoparticulate mercuric halides leading to erroneous measurements. Finally, we estimate airborne mercury aerosols may contribute to half of the oxidized mercury measured in wintertime Montréal urban air using Hg-MS. These emerging mercury-containing nanoparticle contaminants will influence mercury deposition, speciation and other atmospheric and aquatic biogeochemical mercury processes including the bioavailability of oxidized mercury to biota and its transformation to neurotoxic organic mercury.
... Only a few data is published on reactive gaseous mercury (RGM) concentrations in ambient air in China. Using KCl coated tubular denuder technique (Feng et al., 2000), and these limited data showed that RGM concentrations in ambient air of Guiyang were significantly higher than the background RGM concentrations < 10 pg m -3 measured in Northern America and Northern Europe (Lindberg et al., 1998; Sommar et al., 1999). The significant discrepancy of RGM concentrations between the two campaigns is mainly attributed to the weather conditions. ...
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With rapid economy development in China, environmental pollutions from industrialization process are huge concerns though Chinese government has put tremendous efforts to preventi ng emitting pollutants to the environment. China is now regarded as the largest mercury emission country, but the actually mercury pollution status to the environment remains unknown to the rest of the world. After reviewing a great number of papers published in Chinese journals, we summarized the current status of mercury pollutions to surface water, soil and air compartments in China. Anthropogenic mercury inventory from different sources in China in 1995 was estimated according to recent domestic reports and literature data. About 402 metric tons of total mercury was emitted into the atmosphere from China in 1995. The largest atmospheric emission source in China is coal combustion including coal fired power plant and domestic uses, which accounts for 36.1% of total anthropogenic emissions. Tremendously national and international attentions have been given to mercury pollution in the province Guizhou, because of the high geochemical background of mercury in the area and the high mercury emissions from coal combustion using mercury enriched coals as well as from mining activities. Therefore, mercury pollution to the environment in Guizhou is also summarized in this paper.
... Results from two parallel sampling lines are generally concordant, as shown inTable V. The average RGM concentration during the sampling period was 450±250 pg m −3 , which are much higher than that measured at background areas in Europe (Sommar et al., 1999; Feng et al., 2000a) and in U.S.A. (Lindberg and Stratton, 1998). RGM constituted 3.9% of TGM in the air of Guiyang.Figure 5 shows daily average TGM and RGM in the air during the measurement period. ...
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Forty-eight coal samples from the major coal mines in Guizhou were collected by means of subterranean channel sampling. The average mercury content in coal from this Chinese province is 0.53 mg kg-1, which is substantially higher than coal produced in any other province of China. A strong link is proposed to exist between atmospheric mercury emissions and the combustion of coal. During the last two decades, the amount of mercury emitted from coal combustion in Guizhou has increased invariably to 8.3 tons in 1998. Being concentrated to the pyrite fraction in the coal, the implementation of physical coal cleaning is likely to be an effective way to reduce the mercury content. Total and fractionated mercury in air and precipitation was measured in the provincial capital. During a measurement campaign in October 1999, the reactive gaseous mercury (RGM) concentration averaged at 450 pg m-3, which is much higher than that in pristine area (less than 20 pg m-3). The average total mercury in rainwater of 1996 was estimated to be 33 ng L-1, and the total annual wet deposition of mercury in the area was 39 g km-2 in 1996.
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This review critically evaluates the measurement methodologies most commonly employed for the analysis of the various forms of mercury (Hg) in air. Emphasis is given to the three most common forms of mercury in air [i.e. gaseous elemental mercury (GEM, Hg 0), reactive gaseous mercury (RGM), and particle-bound mercury (Hg p)]. Moreover, we also briefly describe methods dealing with gas-phase analysis of organic mercury species (e.g., mostly methyl mercury), as they are also reported to be present in air on rare occasions. To begin with, we describe the approaches to sampling airborne mercury species and associated sample-treatment strategies. We evaluate both conventional and emerging alternative detection techniques for different mercury forms with respect to their applicability in airborne mercury analysis. We also discuss the artifacts and the biases associated with analysis of different mercury species. Finally, the review summarizes current methodological developments for the determination of mercury in air and highlights future prospects for improvements.
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An improved method for the determination of gaseous divalent mercury (GDM) in ambient air using KCl coated denuders has been developed and tested. GDM collected in the KCl coated denuders can be quantitatively desorbed at 450 °C in 10 min. After being complete thermally reduced to Hg0 at 900 °C, all mercury released from the denuder is pre-concentrated on the analytical Au trap, and detected by cold vapor atomic fluorescence spectrometry (CVAFS). The absolute detection limit of the method is less than 3 pg. Preliminary data of GDM concentration in ambient air from different sampling stations show that GDM concentrations in the urban air of Göteborg are much higher than in rural air (Rörvik and Sasetta), which indicates the anthropogenic origin of GDM.
Chapter
Mercury is a fascinating fluid metal that exists as liquid at 25° C and has the lowest known critical temperature (1478° C) (Hensel and Warren, 1999). The dominant form of mercury in atmosphere is the gaseous elemental mercury (Hg(g)) and it is assumed to have a relatively long lifetime (Seiler et al., 1980; Slemr et al, 1985; Lindqvist and Rodhe, 1985). It is speculated that there is about 6,000 tonnes of mercury in the atmosphere, predominantly from anthropogenic origin, such as fuel and coal combustion and waste incineration (UNEP, 2002). Natural emissions, including those from volcanic eruptions, soils, lakes, open water and forest fires, contribute less significantly than anthropogenic sources (ca., 2000 tonnes/yr (Mason et al., 1994) in contrast to 4000 tonnes/yr (Porcella et al., 1997). However, there are significant uncertainties in natural emission inventories (Mason et al., 1994; Gardfeldt, 2003). Atmospheric transformation of mercury can indeed play an important role in the global cycling of this toxic element, as the atmosphere is the fastest moving fluid in the Earth's ecosystem. The atmosphere provides an efficient platform for chemical and physical transformation, as well as short and long-term transport of this pollutant around the globe. The background concentration of atmospheric Hg, which is mainly elemental mercury, in the lower troposphere of the Northern Hemisphere and Southern Hemisphere is around 1.7 and 1.3 ng m-3, respectively (Slemr, 1996; Slemr et al., 2002; Ebinghaus et al., 2002a). Recently it has been reported (Temme et al., 2003) that the fast oxidation of gaseous elemental mercury leads to variable Hg concentrations during the Antarctic summer, accompanied by elevated concentrations, up to more than 300 pg m-3, of reactive gaseous mercury. A major interest in the understanding of atmospheric transformation stems from its potential impact on mercury bioaccumulation. Mercury speciation in the atmosphere has a significant influence on its deposition on environmental surfaces. Solubility and deposition of elemental mercury is quite distinct from Hg+2 (see Table 1), and thus deposition rates on the Earth's surface vary substantially.(Table presented) Methyl mercury has been shown to be biomagnified along food chains. The extent of methylation depends on a constant supply of inorganic mercury from the atmosphere (Mason and Sheu, 2002). Indeed, atmospheric deposition is considered to be a major source of mercury in most remote aquatic systems (Mason et al., 1994; Nriagu and Pacyna, 1988). It is noteworthy that the physicochemical-biological processes that dictate the bioaccumulation of mercury in the food chain have yet to be fully characterized (Morel et al., 1998). Consequently, the extent of incorporation of oxidized mercury produced via atmospheric chemical reactions into the food chain has yet to be evaluated. Figure 1 depicts a simplified schematic of mercury cycling in the Earth's ecosystem and Table 1 illustrates some general physical and chemical properties of mercury compounds of atmospheric interest. (Figure presented) Hg is emitted to the atmosphere from a variety of natural and anthropogenic sources and is removed through dry and wet deposition processes (Lindqvist and Rodhe, 1985). Hg exists in ambient air both in the vapour and particle phase associated with aerosols. Interestingly, in the high-Arctic region (Schroeder et al., 1998), Arctic (Lindberg et al., 2002), and sub-Arctic (Poissant, 2001), the rapid depletion of mercury has been observed. Nearly complete depletions of ozone in the boundary layer occurred over large areas, and evidence of reactive halogens have been observed during most mercury depletion events (MDEs) (Barrie et al., 1988; Jobson et al., 1994; Ariya et al., 1998; 1999). Upon reaction with atmospheric oxidants, elemental mercury can be transformed to its oxidized forms, which are also more bio-accumulative than elemental mercury (Gardfeldt et al., 2001). Observed ozone depletion events at the ground are suggested to be driven by sunlight and bromine atoms derived from reactions of atmospheric reactive halogens with marine sea salt in surface snow and ice (Barrie et al., 1988; Jobson et al., 1994; Ariya et al, 1998; 1999 and 2004). Soon after, mercury depletion was found to be wide spread. Such depletion events have also been observed in the Antarctic (Ebinghaus et al., 2002b), where they are influenced by the photochemical oxidation of elemental mercury in the troposphere involving sea salt on snow/icepack or aerosols (Schroeder and Barrie, 1998; Schroeder et al., 1999; Lu et al., 2001). Unlike the reactions of Hg in solution, experimental data of the gasphase reactions of elemental mercury with some atmospheric oxidants are limited due to the low concentrations of species at atmospheric conditions, the low volatility of products, and the strong effects of water vapour and surface on kinetics. Existence of a dark heterogeneous reaction leading to the formation of Br2 via the oxidation of Br- by O3 has been investigated (Oum et al., 1998). Molecular halogens are photochemically dissociated during polar sunrise, resulting in the production of corresponding atomic species. The halogen atoms further react with ozone, forming halogen oxide radicals (BrO/ClO), which undergo reactions with elemental mercury and transfer them to the oxidized Hg+2 species (Raofie and Ariya, 2004). The primary halogen atoms (Br/Cl) and molecular halogens (Br2/Cl2) may also oxidize elemental mercury to HgBr2, and HgCl2, respectively (Ariya et al., 2002a). The possible reactions of elemental Hg with a variety of atmospheric oxidants and reductants were evaluated using their thermodynamic data by researchers (Schroeder et al., 1991), who then suggested that 0 3 and Cl2 may be important oxidants of Hg, while SO 2 and CO may be important reductants of Hg+2. Both oxidation of Hg and reduction of Hg+2 by H202 are thermodynamically favourable, although literature (Wigfield and Perkins, 1985) indicates the incapability of the oxidation of Hg by H2O2. There have been several excellent review articles on mercury transformation in atmosphere (Linqivist et al., 1999; Schroeder et al., 1991; Lin and Pehkonen, 1999), particularly on its properties, sources, sinks, and fluxes of mercury. As such, in the light of recent laboratory and computational studies, we will attempt to focus instead on a comprehensive review of the kinetic, product studies and thermochemical calculations of gaseous elemental mercury reactions with atmospheric oxidants. We will outline major gaps and some future research directions.
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This article reviews current knowledge of atmospheric mercury processes and describes activities in Europe and North America to simulate these processes by means of tropospheric chemistry/transport models for regional-scale applications. Advantages and limitations of relatively simple Lagrangian models are discussed within the context of issues currently facing the environmental scientific and policymaking communities. The current state and future direction of comprehensive Eulerian models in simulating the tropospheric chemistry and transport of mercury species is outlined. A number of central improvements in these models are discussed, with consideration of the key progress necessary to include feedbacks and interactions between formation and distribution of clouds and mercury atmospheric chemistry.
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A denuder sampling system was developed to measure volatile metals at elevated temperatures. By using the denuder technique it is possible to avoid condensation and adsorption losses in the sampling line. To investigate the behavior of heavy metal species under different physical and chemical conditions, a laboratory scale quartz stack was built. Metal aerosol generators based on evaporation, diffusion and condensation are described. The diameter of the generated particles varied between 0.05-0.3 μm. The day to day reproducibility of the generation varied between 0.6-5.0% for chromium and2.8-4.0% for cadmium (95% stat. significance). Denuders coated by elemental silver seem to be an efficient means for sampling of elemental Cd at 200 °C. The diffusion coefficient of Cd was calculated from experimental data, and the value of (0.42±0.04) cm2/s was obtained. A detection limit of 0.2/μg/m3for Cd determination can be reached by using a Ag-denuder, when a sampling time of 30 min and a flow rate of 601/h is employed.
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The Arctic ecosystem is showing increasing evidence of contamination by persistent, toxic substances, including metals such as mercury1, that accumulate in organisms. In January 1995, we began continuous surface-level measurements of total gaseous mercury in the air at Alert, Northwest Territories, Canada (82.5° N, 62.5° W). Here we show that, during the spring (April to early June) of 1995, there were frequent episodic depletions in mercury vapour concentrations, strongly resembling depletions of ozone in Arctic surface air, during the three-month period following polar sunrise (which occurs in March)2,3.
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Knowledge of atmospheric mercury speciation is critical to understanding its fate once released from point sources. The water-soluble compounds of Hg that exist in flue gases (termed reactive gaseous mercury, RGM) are subject to far greater local removal rates than is elemental Hg vapor, but few ambient air data exist. We developed a method using refluxing mist chambers to quantify the airborne concentrations of RGM in more than 250 1-h samples under ambient conditions and summarize here the results of several RGM sampling campaigns in Tennessee and Indiana from 1992 to 1995. Measured levels of RGM were generally on the order of 50−200 pg/m3, representing about 3% of total gaseous mercury (TGM) and generally exceeding regional particulate Hg concentra tions. RGM exhibits significant correlations (p < 0.05) with temperature, solar radiation, O3, SO2, and TGM, suggesting seasonal trends similar to those of other regional air pollutants. The concentrations of RGM show reproducible diel trends, peaking during midday and decreasing sharply at night. A sharp spike in RGM was measured during a local plume impaction event in Tennessee. Concentration gradients over vegetation suggested a strong ground-level sink for RGM, and RGM concentrations decreased sharply during rain events, as expected for a water-soluble gas. The levels of RGM measured here support the hypothesis that Hg dry and wet deposition may be strongly influenced by the behavior of RGM and that elevated ecosystem exposure may be possible near major point sources of RGM compounds.
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Volatile mercury compounds have been speciated in gases evolved from fermentation of sewage sludge as well as municipal waste. The species were trapped by sequential sampling, using a noble-metal trap in series with an activated-carbon trap. Thermally desorbed Hg0 and (CH3)2Hg were separated by GC at 70 °C and detected by cold vapour atomic fluorescence spectroscopy after thermal reduction. The amounts of mercury detected in the sewage gas correspond to concentrations in the range 50–110 ng m−3 for both species whereas the deposit gases were found to contain only elemental mercury. Monomethylmercury species could not be positively identified in any of the gas samples. Copyright © 1999 John Wiley & Sons, Ltd.
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As part of current efforts to understand the cycling of mercury (Hg) in the atmosphere, information is needed on its atmospheric speciation. Almost no data exists on water-soluble Hg(II) species in ambient air. A new technique for measuring gas phase water soluble Hg(II) species has been developed, utilizing a high-flow refluxing mist chamber. Extensive testing has been carried out, including attempts to rule out production of artifact Hg(II). Measurements at two locations (East-Central Tennessee and the Ohio-Indiana border) found approximately 0.05–0.15 ng/m3 of reactive Hg(II), representing ca. 3 to 5% of the total gaseous Hg. Limited tests of artifact Hg(II) production in the mist chamber by ozone oxidation and co-sampled aerosol Hg(II) suggest that the majority of the collected Hg(II) exists in ambient air in the gas phase.
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Mercury is the only atmospheric pollutant that is present in the atmosphere in atomic form. The optical resonance line at 254 nm can be used for absorption measurements using different optical remote sensing techniques. Range-resolved Hg mapping can be performed using the differential absorption lidar (DIAL) technique. We have used the lidar technique both for mapping of industrial plumes and for background concentration measurements. Our studies also include Hg of geophysical origin.
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Total airborne Hg as well as black particles (soot) were monitored in a number of clean air areas in Sweden. For some of the sampling sites, back trajectories for air movements at 850 mb were provided by the Norwegian Meteorological Institute.It is shown that the total Hg in air may be divided into two fractions. The most important one may be considered to be a background and is probably the result of re-emission of Hg by the ground and by natural water. The other fraction is highly dependent on wind direction in the same way as black particles. This fraction seems to be of anthropogenic origin.
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In an earlier paper (Brosset, 1982) the total Hg in air over Sweden was discussed. The present paper is mainly devoted to oxidized Hg, its origin, transportation and reaction with water. A new nomenclature has been introduced based on the physical properties of Hg-compounds which determine their distribution between air and water and also, as has been the custom hitherto, on their oxidation-reduction properties. It has been established that precipitation contains Hg-salts which are formed through oxidation of metallic vapor in an acid water phase. Rather stable Hg-compounds which seem to be anthropogenic and of the same origin as soot particles are also found in the precipitation.
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Samples for measurements of total gaseous mercury (Hg) in air have been collected since 1980 in south-western part of Scandinavia. A collection program for precipitation samples used to determine changes in depositional fluxes of total Hg has been in operation since 1987. A comparison of today's total gaseous Hg levels in air and the total Hg concentrations in precipitation with the ones found earlier, shows a clear decrease with time. At the Swedish west-coast, yearly average air concentrations and median levels of 3.3 and 3.1 (1980–1984), 3.2 and 2.8 (1985–1989), and 2.7 and 2.6 ng Hg/m3 (1990–1992), respectively, were found. Increased average and median winter concentrations were always found, with levels at 3.7 and 3.4, 3.7 and 3.3, and 3.0 and 2.7 ng Hg/m3 for the respective time period. Higher winter values were expected due to increased anthropogenic emissions and changes in the mixing height of the atmosphere. The corresponding total wet deposition rates decreased from 27 (1987–1989) to 10 g Hg/m2 yr. (1990–1992). A finding of special interest was the decreased number of episodic events of high total gaseous Hg levels in air, from 1990 and further on. In addition, the frequency distribution of the concentrations of Hg in air seems to be different for these years compared to the other two time periods. A frequency distribution of air concentrations of Hg more resembling a normal distribution was found for the years 1990 to 1992. The decrease of the atmospheric burden of total gaseous Hg and deposition of total Hg are most probably connected to lower emissions in source areas on the European continent. It seems logical to state that the problem of high Hg depositional fluxes to Scandinavia, is best solved by abatement strategies on the regional scale.